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 /* NRDF D1547 Data No.17                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,17;
 D#=D1547;
 TITLE=/PROTON SINGLE-PARTICLE STATES IN 21,23NA THROUGH THE
       (D,N) REACTION/;
 PURPOSE=/TO SEE THE SINGLE-PARTICLE OR SINGLE-HOLE STATES IN RESIDUAL
          NUCLEI AND GROUND-STATE PROPERTIES OF THE TARGET NUCLEUS./;
 ATH=(A.TERAKAWA'1',T.TOHEI'1',T.NAKAGAWA'1',A.SATO'1',J.TAKAMATSU'1',
      M.MORI'1',A.NARITA'1',H.ORIHARA'2',K.ISHII'2',T.NIIZEKI'2',
      M.OURA'2',S.HIRASAKI'2',M.HOSAKA'2',G.C.JON'2',K.MIURA'3',
      H.OHNUMA'4');
 INST-ATH=(2JPNTOH'1',2JPNTOH'2',2JPNTOI'3',2JPNTIT'4');
 /*@1@*/
 /*@2@*/
 REF=PR/C;
 VLP=48(1993)2775;
 RCTS=(20NE(D,N)21NA,22NE(D,N)23NA);
 PHQS=(ANGL-DSTRN,SPEC-STR'21');
 /*@22@*/
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 /* Experimental Conditions                                           */
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 \\EXP,17;
 RCT=20NE(D,N)21NA;
 RTY=(INEL-SCATT);
 ENR=99.9%;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=1.0MG/CM**2;
 BAC=SELF;
 ACC=(CYC);
 INST-ACC=2JPNTOH;
 INC-ENGY-LAB=(25MEV);
 CHRG-INC-ION=1;
 DET-PARTCL=(N);
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(TOF)'1';
 /*@12@*/
 SOLID-ANGL=0.23MSR;
 /* EFCN-DET=DETECTOR EFFICIENCY WAS 3% WHICH WAS DETERMINED BY THE
 7LI(P,N)7BE REACTION THROUGH ACTIVATION ANALYSIS. */
 ANL=(OPT-MODEL,ADBA'2',DWBA);
 /*@13@*/
 PHQ=(ANGL-DSTRN,SPEC-STR'21');
 /*@22@*/
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,17;
 INC-ENGY-LAB=25MEV;
 RSD=21NA;
 EXC-ENGY-INITL=2.42MEV;
 J-PTY-INITL=1/2+;
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 /* Data Table                                                        */
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 \DATA;
 THTC'5'  DSIGMA/DOMEGA  DELTA-DSIGMA/DOMEGA
 (DEG)   (B/SR)       (B/SR)
  4.392E+00  3.002E+01  +0.000E+00-0.000E+00
  1.257E+01  8.506E+00  +0.000E+00-0.000E+00
  1.519E+01  4.769E+00  +0.000E+00-0.000E+00
  1.807E+01  1.807E+00  +0.000E+00-0.000E+00
  2.106E+01  1.059E+00  +1.328E-01-1.129E-01
  2.406E+01  1.995E+00  +0.000E+00-0.000E+00
  2.690E+01  2.981E+00  +0.000E+00-0.000E+00
  3.061E+01  3.181E+00  +0.000E+00-0.000E+00
  3.465E+01  2.923E+00  +0.000E+00-0.000E+00
  4.024E+01  1.793E+00  +0.000E+00-0.000E+00
  4.615E+01  6.748E-01  +0.000E+00-0.000E+00
  5.177E+01  1.530E-01  +4.077E-02-2.887E-02
  5.620E+01  1.822E-01  +2.420E-02-1.867E-02
  6.174E+01  3.107E-01  +0.000E+00-0.000E+00
  6.742E+01  4.318E-01  +0.000E+00-0.000E+00
  7.300E+01  4.299E-01  +0.000E+00-0.000E+00
  7.856E+01  3.099E-01  +0.000E+00-0.000E+00
  8.324E+01  1.979E-01  +0.000E+00-0.000E+00
 \END;
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